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higher orbit. Therefore the upper stage doesn’t have to provide as much energy to the<br />

system and can therefore be smaller.<br />

Gross Weight Weight<br />

Dry Dry Weight<br />

Structure<br />

Propulsion Propulsion<br />

Power<br />

Dry Weight Margin<br />

14,270 lb<br />

2,180 lb<br />

1,160 lb<br />

370 lb<br />

130 lb<br />

280 lb<br />

Dry Weight Margin<br />

15%<br />

Power<br />

7%<br />

Propulsion<br />

19%<br />

Figure 35: Weight Breakdown of GT <strong>RASCAL</strong> 2nd Stage.<br />

Structure<br />

59%<br />

The third stage of the GT <strong>RASCAL</strong> also benefits from the weight savings in the<br />

first stage. The third stage is 500 lbs lighter than the baseline. This can be attributed to<br />

the same energy savings as the second stage as well as the fact that a fourth stage has<br />

been added.<br />

Gross Weight<br />

Dry Weight<br />

Structure<br />

Propulsion<br />

Power<br />

Avionics<br />

Dry Weight Margin<br />

2,750 2,750 lb<br />

370 370 lb<br />

110 110 lb<br />

100 100 lb<br />

30 lb<br />

180 180 lb<br />

50 lb<br />

Dry Weight Margin<br />

10%<br />

Avionics<br />

40%<br />

Figure 36: Weight Breakdown of GT <strong>RASCAL</strong> 3rd Stage.<br />

Power<br />

5%<br />

Structure<br />

23%<br />

Propulsion<br />

22%<br />

The Fourth and final stage of the GT <strong>RASCAL</strong> design utilizes a very small<br />

apogee kick motor. This motor is just over 32 lbs with a dry weight of 9lbs. This engine<br />

was sized using a simple two body orbital mechanics as well as the rocket equation<br />

∆ (6)<br />

V = g 0I<br />

sp<br />

ln( MR)<br />

This finite burn is relatively accurate since the circularization burn is very short.<br />

It is also informative to look at the percentage of fuel used in each phase of the<br />

first stages flight (Figure 37). From this figure it can be seen that the majority of the fuel<br />

46

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